david seckel, radio detection of astrophysical neutrinos, karlsruhe, oct. 14, 2003 radio detection...
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David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Radio Detection of Astrophysical Neutrinos
David Seckel
University of Delaware
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Cosmic Neutrinos
• Big Bang < 1 eV Thermal• Solar .1 – 10 MeV Thermonuclear• Supernovae 5 – 50 MeV Thermal
• Atmospheric 100 MeV – 100 TeV Hadronic (-decay)• Cosmic-ray sources1 TeV – 10 EeV Hadronic• Cosmic-ray propagation 100 PeV – 10 EeV P- reactions (GZK)
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Cosmic Rays
• Nuclear (P, Fe?)– ~ E-3 spectrum to 1019 eV
– Sources not observed directly
– GZK process should absorb but…
• Gamma rays– ~ E-2 ’s observed to 1012 eV
– Nearby sources only
• Suggests– E-2 source spectrum
– p,n interact in source
– Predicted fluxes
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Cosmic Ray Neutrinos
production
decay
• Location– Atmosphere
– Source
– Propagation
• Flavor– No mixing
– Full mixing
• If then
Comments
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Expected Fluxes
PP+X
P+
source
GZK
• Waxman - Bahcall– Known intensity
– E-2
– Thin (1 per p)
• But…– Not thin ?
– Didn’t include GZK
• Perhaps WB is better as a lower bound…Anyway - it sets the scale…
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
High energy cross-sections
• ~ E, E < MW2/mp
• Continued increase due to growth
of parton distribution in p,n
• The Earth becomes opaque at
high energy.
* Perhaps non-standard cross-sections – extra dimensions, black holes, etc.
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Detector Scale
Atmospheric 1-100 GeV
Astro-Sources0.1 TeV - 10 PeV
GZK0.1-10 EeV
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Summary of motivation
Source Status Energy Detector Scale
Technology Examples
Atmospheric Observed 1-104 GeV (40 m)3 Water Optical Cerenkov
Super-K
Astrophysical
Sources
Plausible
(but uncertain)
1 PeV 1 km3 Water Optical Cerenkov
IceCube
Antares/Nemo
GZK + “guaranteed” 0.1-10 EeV 1000 km3 Radio Cerenkov
RICE/ANITA
SALSA/GLUE
And lots of more exotic sources, cross-sections, new physics, …
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Radio Detection of Showers
Askaryan: Coherent radiation
• S ~ Q ~ 0.25 Es/GeV• ~ RM ~ 10 cm• /l ~ 3 deg• Confirmed by
– SLAC T444, Saltzberg et al. PRL 2001– SLAC T460, Gorham et al. 2002
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Scaling behavior
fractional excess
V t
lmax
Single particle signal
Includes LPM effect
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
RF spectrum
Field calculation is integral over shower profile
Separation of shower profile
Separation of form factors
With scaled frequencies
• Adapted from Alvarez, Vazquez, Zas
• “Full sim” is approx a
• Blue – Gaussian for f(z), AVZ approx c for Gy
• Red – Griessen for f(z)
Separation of phase factors
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
LPM effect & Hadronic showers
• LPM lengthens shower– Narrows cherenkov cone
• E < 1 EeV e CC showers y = .8• E > 1 EeV hadronic-showers – y = .2
– 3 flavors * (CC + NC) = 4.5 channels– No LPM - no 0 decay above a few PeV (coincidence).
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Radio Propagation in Ice
• Rx fixed• Tx lowered into “dry” hole• t0(z) gives index of refraction• 2nd pulse is reflection
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Radio Attenuation in Ice
0.1 0.2 0.5 1 2 5 10nHGHzL
0.1
1
10
100
1000l
ttaHmkL
lH- 60 CLx 100
lH- 50 CLx 10
lH- 40 CLx 1
Solid – Provorov (used by RICE)Dashed – Matsuoka + Westphal
Curves offset for visibility
RICE bandpass
• High frequency – pretty consistent• Low frequency – big variations with ice sample – proton mobility• Plans to measure at pole, 2003-04
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Radio Ice Cherenkov Experiment
PI
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
RF Detection (RICE version)
5 km
• RF technique– Event
– Shower: EM and/or hadronic
– RF pulse
– Propagation
– Antenna
– DAQ
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
• 16 Rx (10 cm dipole)• 5 Tx• 3 Horns• 4 Oscilliscopes (x4) • DAQ• PCs• Pulse Generator• Dry hole
Pole:
• Network analyzer• Antenna range
Kansas:
RICE Deployment
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Channel and DAQ configuration
Power
Scope
Trigger generator
Antenna
Amp in PV
cableAmpFilter
Splitter
PC• 4 hits within 1200 ns • Latch scope• TDC times to PC • On-line veto (TDC times)
• Read scope• Write to disk
• 8 sec• 1 ns sample• 500 MHz
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Single Channel Calibrations
200-500 MHz: +/- 3 dB (E)
TX….RX • antenna + amplifier calibrations• cable (TX, RX) and filter• relative geometry of TX/RX (r,
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Pulse shape simulation
Disc. threshold
Background taken from data sample
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Limited by attenuation
60,000 e- showers at E = 1 EeVBlack dots – sampleRed dots – events which would trigger RICE
~ 5% efficiency
Limited by Cherenkov angle
Monte Carlo
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
1. 2. 3. 4. 5. 6.Log@EsDHPeVL- 3.
- 2.
- 1.
0.
1.
2.
goL@V ffeDHmk3 L
RICE effective volume for e-, showers
Range due to varyingsignal strength by 0.5-2
Range due to varyingattenuation by 0.5-2
Mul
tipl
y by
2
sr
This is appropriatefor e chargedcurrent events.
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
1. 2. 3. 4. 5. 6.Log@EsDHPeVL- 3.
- 2.
- 1.
0.
1.
2.
goL@V ffeDHmk3 L
LPM and hadronic showers
With LPMWithout LPM
“Hadronic”Es = 20% E
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
RICE I: Data Analysis
333.3 hrs livetime
TDC times
Waveform
data {
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
No Events! (yet)
ICRC 2003
SPIE 2002Astro-ph 2002
AstroPart Phys.2003
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Potential Systematic Effects (see astro-ph/0206371)
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
ANITA
Peter Gorham
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Antarctic Impulsive Transient Antenna (ANITA)
• ANITA Goal: Pathfinding mission for balloone-borne neutrino telescope
• NASA SR&T start 2003, LDB launch in `06-`07 austral summer season
• Requires early measurements of Antarctic EMI at float altitudes determines instrument final design
M. R
osen, Univ. of
Haw
aii
ANITAGondola &
Payload
Antenna array
Crush pad/struts not shown
Solar Panels
Mean ice depth ~1.2km
SIP & SIP PV array
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Critical Developments
• Broad band antennas with 30 deg field of view, two polarizations
• Survey of EMI backgrounds – ANITA Lite
• Low power multichannel digitizer
– >= 1GHz analog input bandwidth (200-1200MHz)– multi-GSa/s sampling rate (Nyquist limit ideal)– minimum phase distortion for clean polarization – dynamic range (>= 10 bits)– internal Analog to Digital Conversion (ADC)– short record length (100-200ns if optimally matched)
– self-triggering with fine threshold adjustment– bi-polar triggering– deadtimeless conclude multi-hit buffering needed
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
32x256 SCA bank
DACs ADC
Trigger
scalers
STRAW2 Chip
16 Channels of256 deep SCA buckets
Self-Triggered Recorder Analog Waveform (STRAW)
Optimized for RF inputMicrostrip 50
Record length:128-256ns
Self-Triggering:
Target input Bandwidth:>700MHz
-LL and HL (adj.) for each channel
Sampling Rate:1-2GSa/s (adj.)
-Multiplicity trigger for LL hits
On-chip ADC:12-bit, >2MSPS
External option:MUXed Analog out
Sampling Rates>~8GSa/s possiblew/ 0.25m process
8192 analog storage cells
Die:~2.5mm2
(From Gary Varner, UH)
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
ANITA MC
• Ec = 3e18 eV
• 5.6 deg upcoming
• 100m depth
• Ec = 2.5e18 eV,
• 0.7 deg upcoming
• depth 950m
~30 deg
~45 deg
• Method: monte carlo ray bundles from ZHS distribution, then ray-trace through the ice+firn to surface, then use fresnel equations
• Also extending RICE Monte Carlo
• Issue: Roughness of Air-Ice interface
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Current best sensitivity estimates
From: Peter Gorham
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Anita-lite Configuration (w/TIGER)
• 2 quad-ridged horn antennas on SIP level
• Electronics 1atm case (also SIP level)
• PV array addition
• Telemetry integrated w/ TIGER
marriage made in heaven (Lady & the tiger)
Anita-lite PV array:Probably integrated in single
tier
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
ANITA-lite as-built Configuration
Antenna arrangement
Instrument housing under TIGER
Redundant fast-recovery USB harddrive (8GB)Housing, hard drive, veto antenna
Electronics integration into pressure housing
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Air Shower Detection
• Demonstration that Radio Cerenkov works “in the wild”
• Detector Calibration
• Cosmic ray composition ?
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Impact of shower core
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
RF pulse: rant= (0,0,-150m), dsh= +x on cone
Arrival time distribution
RF Pulse at antenna Combined spectra w/phases
Individual spectra above 300 GeV
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Different pulse shapes for different observers
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Compare strength of air/ice shower signals
-4 -2 0 2 4tns-0.00002
0
0.00002
0.00004
0.00006
EVmmc
PeV ice shower x .01redvs PeV Air shower black • Need to correct for constant n = 1.78
– Narrower C-cone
– Increases E
– No focusing
• Vertical shower– Slant will evolve shower
• Higher E more efficient– Will penetrate (less evolved)
• Proton vs Fe– Fe more evolved - larger H
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Plausible event rates
• A = 1 km2
• Impact Rates– Es > 1 PeV = 108/yr
– Es > 1 EeV = 102/yr
• Threshold– E (in ice) ~ 300 PeV (RICE)
– E (in ice) ~ 10 PeV (Optimized ?)
• Need MC of air shower rates, array design– Toy calc with RICE
• 10 EeV air shower, r = 2 km, z < 45
• 0.1 EeV ice shower, z = 1 m (w/LPM)
• No ray tracing (change geometry/strength)
• eff ) = 1.9 km2sr
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Composition with radio ?
Proton gammaFe
Average of 50 x 1 PeV showers
David Seckel, Radio Detection of Astrophysical Neutrinos, Karlsruhe, Oct. 14, 2003
Summary
• Cosmic Rays & Neutrinos linkedOther cosmic neutrinos/particle physics not discusse
• RF detection offers large effective volumes
• RICE maturing as a prototype
• ANITA discovery potential designed for GZK
• Air shower detection w/composition ?